Quiescent H-mode: Difference between revisions
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A Quiescent H-mode is an [[H-mode]] without [[Edge Localized Modes|ELM]] activity. | A Quiescent H-mode is an [[H-mode]] without [[Edge Localized Modes|ELM]] activity. | ||
<ref>[[doi:10.1088/0741-3335/44/5A/325|K.H. Burrell, M.E. Austin, D.P. Brennan, et al., ''Quiescent H-mode plasmas in the DIII-D tokamak'', Plasma Phys. Control. Fusion '''44''' (2002) A253]]</ref> | <ref>[[doi:10.1088/0741-3335/44/5A/325|K.H. Burrell, M.E. Austin, D.P. Brennan, et al., ''Quiescent H-mode plasmas in the DIII-D tokamak'', Plasma Phys. Control. Fusion '''44''' (2002) A253]]</ref> | ||
The absence of ELMs is positive | <ref>[[doi:10.1103/PhysRevLett.102.155003|K.H. Burrell, T.H. Osborne, P.B. Snyder, et al., ''Quiescent H-Mode Plasmas with Strong Edge Rotation in the Cocurrent Direction'', Phys. Rev. Lett. '''102''' (2009) 155003]]</ref> | ||
The absence of ELMs is positive as it reduces stresses on and damage to plasma facing components (mainly the [[divertor]]), | |||
but inconvenient from the point of view of impurity accumulation. | but inconvenient from the point of view of impurity accumulation. | ||
== References == | == References == | ||
<references /> | <references /> | ||
Revision as of 07:29, 28 July 2012
A Quiescent H-mode is an H-mode without ELM activity. [1] [2] The absence of ELMs is positive as it reduces stresses on and damage to plasma facing components (mainly the divertor), but inconvenient from the point of view of impurity accumulation.
References
- ↑ K.H. Burrell, M.E. Austin, D.P. Brennan, et al., Quiescent H-mode plasmas in the DIII-D tokamak, Plasma Phys. Control. Fusion 44 (2002) A253
- ↑ K.H. Burrell, T.H. Osborne, P.B. Snyder, et al., Quiescent H-Mode Plasmas with Strong Edge Rotation in the Cocurrent Direction, Phys. Rev. Lett. 102 (2009) 155003